|Publication number||US6072765 A|
|Application number||US 09/263,008|
|Publication date||Jun 6, 2000|
|Filing date||Mar 5, 1999|
|Priority date||Jul 28, 1997|
|Also published as||US5921926, US6141577|
|Publication number||09263008, 263008, US 6072765 A, US 6072765A, US-A-6072765, US6072765 A, US6072765A|
|Inventors||Jannick P. Rolland, Peter J. Delfyett, Jr.|
|Original Assignee||University Of Central Florida|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (16), Non-Patent Citations (28), Referenced by (39), Classifications (20), Legal Events (5)|
|External Links: USPTO, USPTO Assignment, Espacenet|
This is a Divisional Application of application Ser. No. 09/002,069 filed Dec. 31, 1997, now U.S. Pat. No. 5,921,926, issued on Jul. 13, 1999.
This invention relates to imaging devices, and in particular to a probe that simultaneously performs optical coherence tomography(OCT) and spectral analysis using back reflected light. The probe and attached instrumentation performs three dimensional imaging of cavity interior walls such as but not limited to a uterus/cervix body area for detecting cancerous tumors. This is a Continuation-In-Part of Provisional Application 60/053960 filed on Jul. 28, 1997.
Pap smears have been used regularly for diagnosing cervical cancer. Pap smear tests have an approximately 70% sensitivity (true positive/total number of actual abnormal cases. Generally when using a Pap smear for diagnosing cervical cancer, internal tissue areas in the cervix are scraped and analyzed by a microscope to check for abnormal tissues.
Following an abnormal Pap smear, a patient is recommended for a more in depth examination by a gynecologist specializing in cancer, including cancer of the female genital track. Colposcopy (i.e., observation of the cervix) is typically performed on the patient. During colposcopy, a colposcope (a magnifying microscope) is used to attempt to identify suspect lesions. A colposcope image of the cervix is reproduced at a remote distance from the patient. Subsequent to colposcopy, biopsy of suspected lesions is commonly performed for histology follow up. When a biopsy is performed, several tissue samples are cut-out and sent to a cytology laboratory for further analysis. While there are various classifications for degree of cell abnormality, an abnormal lesion can include atypical cells, virus infected cells such as human papilloma, pre malignant cells, and malignant cancer cells.
There are several problems with using the Pap smear first followed by either or both the biopsy and/or the colposcopy. Patient compliance is a major problem to having a biopsy performed. Patients have been known to procrastinate and delay these follow-up procedures because of fear of having a biopsy. This time delay hurts the chance of recovery, since cancer is best treated in its earliest stage. Problems are further compounded because every time abnormal cells are detected during a Pap smear, there has to be another colposcopy and another biopsy. Repeating Pap smears followed each time by colposcopy and biopsy increases the odds of not obtaining patient compliance. Additional problems exist with pregnant patients, because biopsy is not recommended during pregnancy due to the increased risk of bleeding.
Inventions have been proposed for overcoming these problems, but still fail to adequately cover all of these problems with a single procedure. See for example U.S. Pat. No. 5,179,937 to Lee; U.S. Pat. No. 5,321,501 to Swanson et al.; 5,451,785 to Faris; U.S. Pat. No. 5,458,595 to Tadir et al.; U.S. Pat. No. 5,465,147 to Swanson; U.S. Pat. No. 5,467,767 to Alfano et al.; U.S. Pat. No. 5,491,524 to Hellmuth et al.; U.S. Pat. No. 5,496,305 to Kittrell et al.; U.S. Pat. No. 5,507,287 to Palcic et al.; U.S. Pat. No. 5,537,162 to Heilmuth et al.; U.S. Pat. No. 5,558,669 to Reynard; U.S. Pat. No. 5,573,531 to Gregory; and U.S. Pat. No. 5,591,160 to Reynard. U.S. Pat. Nos. 5,321,501 and 5,451,785 to Swanson are the closest prior art devices that mention it may be desirable to scan tissue inside tubular structures such as genital tracts. However, these patents do not conduct imaging and spectroscopy simultaneously.
A primary objective of the present invention is to use a coherence scanning microscope for the diagnosis of surface tissues such as, but not limited to, skin and cervical tissues, in vivo.
The second objective of the present invention is to use optical coherence tomography (OCT) in a probe for three dimensional imaging of a uterus/cervix area for cancer detection
The third objective of the present invention is to provide a tunable source of low-coherence light to simultaneously conduct spatial imaging and spectral sensing for tissue diagnosis.
The fourth objective of the present invention is to provide real-time three-dimensional colposcopy diagnosis.
The fifth objective of the present invention is to provide an automatic means to guide surgery when cancer has been detected.
The sixth objective of the present invention is to provide guidance to physically biopsy suspicious sites during colposcopy.
Further objects and advantages of this invention will be apparent from the following detailed description of a presently preferred embodiment which is illustrated schematically in the accompanying drawings.
FIG. 1 is a perspective view of a first preferred embodiment of the novel probe and receiver device for simultaneous acquisition of spatial and spectral OCT (SI-OCT).
FIG. 2 is an enlarged view of the rear portion of the probe of FIG. 1.
FIG. 3 is a perspective view of a second embodiment of a SI-OCT interferometer and parallel detector acquisition system used with the probe of FIG. 1.
FIG. 4 is a schematic view of a third embodiment for optical memory readout using low coherence tomography and spectral interferometry using the detectors of the preceding figures.
Before explaining the disclosed embodiment of the present invention in detail it is to be understood that the invention is not limited in its application to the details of the particular arrangement shown since the invention is capable of other embodiments. Also, the terminology used herein is for the purpose of description and not of limitation.
FIG. 1 is a perspective view of a first preferred embodiment 1 of the novel probe 150 and receiver 5. Each of the components of FIG. 1 will now be described. Fiber splitter 80 can be a 50%/50% fiber splitter such as a JDS Fitel or a Corning component. The low-coherence light source 30 can be continuous or chirped source from emitting diodes(LED), superluminance laser diodes(SLDs), multiple light emitting diode, or a modelocked laser, such as in U.S. Pat. No. 5,469,454 by one of the co-inventors of the subject invention, which is incorporated by reference.
Electronics 50 can be an envelope detector, or a demodulation circuit. Detector 60 can be a single detector such as a silicon power meter or a detector array such as a silicon CCD detector array, manufactured by for example, but not limited to Sharp, Toshiba, and NEC. Fiber Splitters 70 and 80 can be a 50%/50% fiber splitter. Spectrometer 90 can be a Jarred-Ashe 3/4 meter spectrometer, or an Ocean Optics Spectrometer. CCD Detector 91 can be a linear silicon detector array such as detector 60 manufactured by Sharp, Toshiba, and NEC. Computer 100 can be an EBM586 compatible such as a Dell, Gateway or Compaq computer.
The computer 100 can be used to perform a 3D-image reconstruction from raw or processed data. 3D rendering of reconstructed data, and 3D visualization of rendered data. In the same way that color can be tagged with a saturation parameter and a hue parameter, the amplitude of the back scattered Light as well as its spectral signature will serve a tag parameter for the 3D data volume being sensed. OCT imaging can provide the amplitude of the back scattered light at each spatial location (x,y,z), which can be assembled in a 3D matrix that can be displayed as a 3D volume. Software used in computer 100, can be any programming language such as a C, C++, Fortran, IDL, which can visualize the 3D data either as cross sections (x, y) of the tissue or as a volume using various visualization techniques such as transparency rendering, volume rendering, and the like. Similarly, the spectral data can be visualized separately and one or several parameters from the spectral analysis can be extracted. Those parameters can also serve as a tag to the spatial data. Moreover, spectral data can be used in processing the spatial data as data provides information about the dispositives of the medical condition. Finally, data fusion of spatial and spectral information can be performed as yet another way to visualize the data.
Delay line 110 can be an adjustable optical delay using a stepper motor and optical flat or retroreflecting mirror, or microreflector sheet, a mirror made of reflector tubes, or an helicoid rotating mirror, or an expanding fiber optic cylindrical solenoid. The collimated lens 120 can be a fiber optic collection lens cemented or not to the fiber with for an example, a 0.1 numerical aperture or equivalently an F-number of 5. The reference Mirror 130 can be a flat silver, gold, or dielectric mirror manufactured by Newport for example. Single mode fiber 145 is an approximately 5 micron to approximately 10 micron core optical fiber with optional polarization preserving. Under polarization preserving light entering the optical fiber with a given state of polarization(such as vertically polarized) exits from the optical fiber with the same state of polarization(i.e. vertically polarized).
Referring to FIG. 1, axially rotating probe 200 includes a scanning mirror and the fiber optics array, and a lenslet array, shown in more detail in reference to FIG. 2. Optoelectronics scanners providing random access scanning acousto-optics scanners, can also be used instead of a mirror. Plastic lenslet array 155 can have an approximately 0.1 numerical aperture and approximately 200 micron center to center spacing. Planar fiber optics array 160 is a coherent linear fiber bundle in one plane where a multiplicity of optical fiber is laid down, one by one next to each other forming one layer or one plane. A disposable plastic envelope 170 encompasses optics array 160, and a disposable sealed plastic lenslet array 180 such as that described in reference to 155 is across the front face of envelope 170
A speculum 195, currently used in medical practice to do either a Pap smear or colposcopy, such as the one described in U.S. Pat. No. 5,179,937, which is incorporated by reference, is used for vaginal inspection, so that probe 200 can allow for imaging of the endocervical canal 192 and the face of the cervix 194.
FIG. 2 is an enlarged cross-sectional view of the rear portion 200 of the probe 150 of FIG. 1. Incoming optic fiber 147 from main receiver 5 is shown in FIG. 1. Referring to FIG. 2, electrical wire bundle 149 can be a group of electrical wires which carry current for powering servo motor 230. An outer casing 202 such as an aluminum box can contain the probe-optical scanning components. Screw type fasteners 207 fasten DC servo motor 205 to the casing 202, and motor head gear 210 allows cylinder 240 to rotate within casing 202. Cylindrical bearings 215 are a metal type cylinder that prevents the translation of the probe 200. A single mode optical fiber 220 extends into the interior of probe 200. Cylinder 240, lens array 155 and planar optical fiber array 160 rotates in the direction or counter direction of arrow B about the central axis of rotation 225. Servo motor 230 can be another DC servo motor similar in operation to motor 205 described above. Mirror 235 can be a metal or dielectric highly reflecting mirror, and the rotating cylinder 240 can be a hollow metal cylinder.
The above described components allow for simultaneous OCT and spectral imaging for cancer diagnosis of the cervix. Because of the low coherence of the light source used for OCT imaging, back scattered light only interferes constructively, that is adds, when the optical path length difference between the light path to the reference mirror 130, and that to the sample 192, 194 is less than the coherence length of the light. Therefore, as the optical path length to the mirror shortens or expands as a result of the z-scan done by the reference mirror 130 in our embodiment, the image depth in the tissue that can produce constructive interference with the reference path is that for which the optical path length is equal to the referenced beam with a precision of the coherence length of the light source. Scan can be performed by various scanning schemes including a moving mirror 235 rotatable in the direction of arrow C or expending piezoelectric solenoid on which the optical fiber is enrolled. Typically, resolutions in z of 10-13 microns can be achieved with current OCT systems. While this interferometric principle, which is nothing more than the Michelson interferometer principle first demonstrated in the 1800's which, in its utilization for biological tissue sensing, one must operate at a wavelength or a set of wavelength where the tissue is transparent to the light, meaning there is little or no absorption. The fundamental principle has also been referred as an coherent microscope principle before OCT was named as such. The subject invention uses a broad spectrum wavelengths from 0.4 μm to 1.3 μm. For the spectral analysis, various wavelength can be used depending on the type of analysis. For spectral interferometry visible or infrared light can be used. For fluorescence spectroscopy, one will also want to operate in part in the blues, at approximately 0.4 μm.
FIG. 3 is a perspective view of a second embodiment 300 of a interferometer and parallel detector acquisition system used with the probe of FIG. 1. The components of FIG. 3 will now be described. Tunable low coherent optical source 310 can be a spectrally broad band light, LED, modelocked laser or chirped pulse light source. The low coherence light source 320 can be a light emitting diode or equivalent type source. Collimating lens 330 and 360 can be positive lens (plastic glass) or lenslit array. Collimating lens 330 is used to collimate light from light source 310 and 320. Collimating lens 360 is used to collimate light impinging on the reference mirror 370 back into the fiber 350. Fiber optic bundles 340, 350, 353 and 350' can be 2-D coherent fiber bundles. Reference mirror 370 is similar to reference mirror 235 described previously. Reference Mirror 370 can be replaced by a micro-lenses of retro-reflectors, or other types of mirrors such as those described previously, for redirecting light. The Light coupling lenslit arrays 380 can be a micro lenses arranged in a 2-D array to collect and collimate light to beam splitter 381. Fiber splitter 390 can be a 50%/50% fiber splitter that directs light to a CCD detector array 410(similar to detector 60 previously described) and to the spectrometer 400(similar to 35 previously described). Electronics 420 is equivalent to previously described electronics 50 which can be an envelope detector, a demodulator circuit, and the like. Computer 430 is equivalent to computer 100 described previously.
In this configuration of incorporating FIG. 3 into the probe 200 of FIG. 2, the light source is collimated and fed in parallel to the fiber optic bundle 340. Upon exiting fiber 340, the light is coupled into the fiber bundles 350 and 353 via lenslet arrays glued to the beam splitter 381. On the reference path, the light exiting the bundle array 350 is collimated before it is reflected by the reference mirror 370. Upon reflection, the light is coupled back to the same fiber bundle 350. It is then reflected at the half silvered surface of the beam splitter 381 which corresponds to the diagonal line in the middle of element 381. The light is then directed using fiber bundle 353 (the one going down) in part to the CCD detector array 405 and in part to the spectrometer 400. On the sample path, the light reflected upward (in this case) the beam splitter goes to the in vivo biological tissue to be diagnosed. Light is reflected back in parallel from the surface of the tissue and all layers of the tissue, but only the tissue at the depth corresponding to the equivalent optical path for the reference beam will be detected. This configuration allows parallel processing on information. Because of the limitation in resolution of current technology fibers, samples separated 100 to 200 micron apart are imaged simultaneously. By allowing transversal scan of the overall probe assembly resolution to sub fiber sizes can be obtained. If fibers are separated by 100 microns, for example, 10 transversal scan values can allow 10 microns transversal resolution. With nanotechnology of the future no transversal scan will be necessary.
FIG. 4 is a schematic view of a third embodiment 500 for optical memory readout using low coherence tomography and spectral interferometry using the detectors of the preceding figures. Embodiment 500 encompasses a multi-layer optical disk readout using low coherence tomography and spectral interferometry. The concept of optical disk readout using OCT, or optical coherence tomography is similar to that employed in imaging techniques. The salient feature is to measure the cross-correlation function from the reflected Light returning from a multilayer compact optical disk. The locations of the peaks in the correlation function uniquely determine the bit pattern recorded on the optical disk as a function of depth within the disk. Alternatively, by employing spectral interferometry, the measured optical spectrum also provides a unique mapping of the recorded bits onto the observed spectral modulation. The unique feature is that by simultaneously employing both spectral interferometry and low coherence tomography, the resultant data transfer rate is increased, and the combination also allows for error rate analysis. Similarly for medical diagnosis, combing OCT and spectral OCT or spectroscopy will for higher sensitivity and specificity than obtained or either method alone.
Referring to FIG. 4, embodiment 500 includes a low coherence light source 510. Low coherence light source 510 can be an LED or superluminescent laser diode having a wavelength of approximately 830 nm. Component 520 can be a partially silvered mirror or a beam splitter. Movable mirrors 530 and 560 with length adjustment can be a dielectric or metal highly reflective mirrors. Detector or spectrometer with detector array 550 can be a Jarred Ashe spectrometer and linear silicon diode detector array. Multilayer compact optical disk 570 can be a layered dielectric mirror with recorded pits and lands.
The low coherent light source 510 generates the light to be used in the low coherence memory application. The light is collected and collimated and directed to a 50%/150% beam splitter 520. The two beans generated from the beam splitter are directed to a mirror 530, 560 with a length adjustment and to the multilayer compact optical disk. Light is reflected from the mirror 530, 560 with length adjustment and the compact optical disk. It should be noted that owing to the separate, individual layers within the optical disk, a portion of the light is reflected from each layer. The reflected light from both the movable mirrors 530, 560 and from each layer within the compact optical disk 570 is recombined back on the beam splitter 520. The recombined light at 555 is then measured using a detector or spectrometer 550 with a detector array. By adjusting the optical path length using the movable mirror, the resulting interference, or correlation function, is measured. It should be noted that each peak in the correlation function provides information as to whether there is a recorded pit or land, corresponding to a logical 1 or 0, at a specific location on the optical disk. Alternatively, by measuring the spectral interference fringe pattern using the spectrometer and the detector array 550, the spectral pattern yields a unique distribution which corresponds to the data bits recorded at each level in the disk at a specific location.
By collecting the correlation, or spectral interferometry, data at each position on the multilayer optical disk 570, one extracts the data recorded at each location and on each layer within the optical disk.
While the invention has been described, disclosed, illustrated and shown in various terms of certain embodiments or modifications which it has presumed in practice, the scope of the invention is not intended to be, nor should it be deemed to be, limited thereby and such other modifications or embodiments as may be suggested by the teachings herein are particularly reserved especially as they fall within the breadth and scope of the claims here appended.
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US5179937 *||May 28, 1991||Jan 19, 1993||Lee Chenault D||Disposable vaginal speculum|
|US5321501 *||Apr 29, 1992||Jun 14, 1994||Massachusetts Institute Of Technology||Method and apparatus for optical imaging with means for controlling the longitudinal range of the sample|
|US5451785 *||Mar 18, 1994||Sep 19, 1995||Sri International||Upconverting and time-gated two-dimensional infrared transillumination imaging|
|US5458595 *||Dec 16, 1993||Oct 17, 1995||The Regents Of The University Of California||Vaginal speculum for photodynamic therapy and method of using the same|
|US5465147 *||Jun 2, 1994||Nov 7, 1995||Massachusetts Institute Of Technology||Method and apparatus for acquiring images using a ccd detector array and no transverse scanner|
|US5467767 *||Aug 27, 1993||Nov 21, 1995||Alfano; Robert R.||Method for determining if tissue is malignant as opposed to non-malignant using time-resolved fluorescence spectroscopy|
|US5491524 *||Oct 5, 1994||Feb 13, 1996||Carl Zeiss, Inc.||Optical coherence tomography corneal mapping apparatus|
|US5496305 *||Jan 29, 1992||Mar 5, 1996||Massachusetts Institue Of Technology||Catheter for laser angiosurgery|
|US5507287 *||Apr 27, 1995||Apr 16, 1996||Xillix Technologies Corporation||Endoscopic imaging system for diseased tissue|
|US5537162 *||Dec 17, 1993||Jul 16, 1996||Carl Zeiss, Inc.||Method and apparatus for optical coherence tomographic fundus imaging without vignetting|
|US5558669 *||Jun 22, 1995||Sep 24, 1996||Reynard; Michael||Fiber optic sleeve for surgical instruments|
|US5573531 *||Jun 20, 1994||Nov 12, 1996||Gregory; Kenton W.||Fluid core laser angioscope|
|US5591160 *||Jun 5, 1995||Jan 7, 1997||Reynard; Michael||Fiber optic sleeve for surgical instruments|
|US5710752 *||Jun 7, 1995||Jan 20, 1998||Dolby Laboratories Licensing Corporation||Apparatus using one optical sensor to recover audio information from analog and digital soundtrack carried on motion picture film|
|US5784352 *||Aug 19, 1997||Jul 21, 1998||Massachusetts Institute Of Technology||Apparatus and method for accessing data on multilayered optical media|
|US5921926 *||Dec 31, 1997||Jul 13, 1999||University Of Central Florida||Three dimensional optical imaging colposcopy|
|1||*||Boppart, et al., Investigation of Developing Embryonic Morphology using Optical Coherence Tomography, Developmental Biology , 1996, vol, 177, pp. 54 63.|
|2||Boppart, et al., Investigation of Developing Embryonic Morphology using Optical Coherence Tomography, Developmental Biology, 1996, vol, 177, pp. 54-63.|
|3||*||Bouma, et al., High Resolution Optical Coherence Tomographic Imaging Using a Mode Locked Ti: A12 0 3 Laser Source, Optical Society of America , Jul. 1, 1995, No. 13, pp. 1486 1487.|
|4||Bouma, et al., High-Resolution Optical Coherence Tomographic Imaging Using a Mode-Locked Ti: A12 0 3 Laser Source, Optical Society of America, Jul. 1, 1995, No. 13, pp. 1486-1487.|
|5||*||Brunner, et al., Optical Coherence Tomography (OCT) of Human Skin with a Slow Scan CCD Camera, SPIE , vol. 2626, pp. 273 282.|
|6||Brunner, et al., Optical Coherence Tomography (OCT) of Human Skin with a Slow-Scan CCD-Camera, SPIE, vol. 2626, pp. 273-282.|
|7||*||Chan, Imaging Through Biological Tissues by use of Optical Low Coherence Heterodyne Detection Technique, AMF , 20, pp. 119 130.|
|8||Chan, Imaging Through Biological Tissues by use of Optical Low-Coherence Heterodyne Detection Technique, AMF, 20, pp. 119-130.|
|9||*||Fercher, et al., Eye Length Measurement by Interferometry with Partially Coherent Light, Optical Society of America, Mar. 1988, vol. 13, No. 3, pp. 186 188.|
|10||Fercher, et al., Eye-Length Measurement by Interferometry with Partially Coherent Light, Optical Society of America, Mar. 1988, vol. 13, No. 3, pp. 186-188.|
|11||*||Hee, et al., Femtosecond Transillumination Optical Coherence Tomography, Optical Society of America , Jun. 15, 1993, vol. 18, No. 12 pp. 950 952.|
|12||Hee, et al., Femtosecond Transillumination Optical Coherence Tomography, Optical Society of America, Jun. 15, 1993, vol. 18, No. 12 pp. 950-952.|
|13||*||Hodson, et al., Detecting Plant Silica Fibers in Animal Tissue by Confocal Fluorescence Microscopy, Elsevier Science Ltd., 1994, vol, 38, No. 2 pp. 149 160.|
|14||Hodson, et al., Detecting Plant Silica Fibers in Animal Tissue by Confocal Fluorescence Microscopy, Elsevier Science Ltd., 1994, vol, 38, No. 2 pp. 149-160.|
|15||*||Jones, Real Time Three Dimensional Imaging Through Turbid Media using Photorefractive Holography, AMC , 4, pp. 27 32.|
|16||Jones, Real-Time Three Dimensional Imaging Through Turbid Media using Photorefractive Holography, AMC, 4, pp. 27-32.|
|17||*||Maki, Spatial and Temporal Analysis of Human Motor Activity Using Non invasive Optical Topography, AMF , 24, pp. 131 132.|
|18||Maki, Spatial and Temporal Analysis of Human Motor Activity Using Non-invasive Optical Topography, AMF, 24, pp. 131-132.|
|19||*||Milner, Low Coherence Interferometry as a Biomedical Monitor in Skin, Tearney, et al., High Speed Optical Coherence Tomography, Kulkarni, et al., High Resolution Optical Coherence Tomography using Deconvolution, Boppart, Optical Coherence Tomography of Embryonic Morphology during Cellular Differentiation, Gleyzes, et al., A Multichannel Approach to Coherent Optical Imaging Through Trubid Media, Was, Heterodyne Measurement of Winger Phase Space Distributions in Turbid Media, Coherence Imaging Techniques 11, Mar. 20, 1996, Russian Academy of Science.|
|20||*||Schmidt, et al., Measurement of Optical properties of Biological Tissues by Low Coherence Reflectometry, Applied Optics , Oct. 1993, vol. 32, No. 30, pp. 6032 6042.|
|21||Schmidt, et al., Measurement of Optical properties of Biological Tissues by Low-Coherence Reflectometry, Applied Optics, Oct. 1993, vol. 32, No. 30, pp. 6032-6042.|
|22||*||Sergeev, et al. Biomedical Diagnostics using Optical Coherence Tomography, Brezinski, et al. High Resolution Intraarterial Imaging with Optical Coherence Tomography, Izatt, et al.., Optical Coherence Tomography and Microscopy in Gastrointestinal Tissues, Coherence Imaging Techniques 1, Mar. 18, 1996, University of Pennsylvania.|
|23||*||Swanson, et al., High Speed Optical Coherence Domain Reflectometry, Optics Letters , Jan. 1992, vol. 17, No. 2, pp. 1864 1865.|
|24||Swanson, et al., High-Speed Optical Coherence Domain Reflectometry, Optics Letters, Jan. 1992, vol. 17, No. 2, pp. 1864-1865.|
|25||*||Takada, et al. New Measurement System for Fault Location in Optical Waveguide Devices Based on an Interferometric Technique, Applied Optics , May 1, 1987, vol. 26 No. 9, pp. 1603 1607.|
|26||Takada, et al. New Measurement System for Fault Location in Optical Waveguide Devices Based on an Interferometric Technique, Applied Optics, May 1, 1987, vol. 26 No. 9, pp. 1603-1607.|
|27||*||Zhou, et al. Prospects of Using an IVEM with a FEG for Imaging Macromolecules Toward Atomic Resolution, Elsevier Science Publishers, 1993, pp. 408 416.|
|28||Zhou, et al. Prospects of Using an IVEM with a FEG for Imaging Macromolecules Toward Atomic Resolution, Elsevier Science Publishers, 1993, pp. 408-416.|
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US6763149||Apr 24, 2002||Jul 13, 2004||Amnis Corporation||Method and apparatus for correcting crosstalk and spatial resolution for multichannel imaging|
|US7006710||Feb 20, 2004||Feb 28, 2006||Amnis Corporation||Method and apparatus for correcting crosstalk and spatial resolution for multichannel imaging|
|US7023563||Feb 14, 2003||Apr 4, 2006||Chian Chiu Li||Interferometric optical imaging and storage devices|
|US7184148||May 14, 2004||Feb 27, 2007||Medeikon Corporation||Low coherence interferometry utilizing phase|
|US7190464||Jan 21, 2005||Mar 13, 2007||Medeikon Corporation||Low coherence interferometry for detecting and characterizing plaques|
|US7242480||Jan 21, 2005||Jul 10, 2007||Medeikon Corporation||Low coherence interferometry for detecting and characterizing plaques|
|US7327463||May 14, 2004||Feb 5, 2008||Medrikon Corporation||Low coherence interferometry utilizing magnitude|
|US7474408||Oct 25, 2006||Jan 6, 2009||Medeikon Corporation||Low coherence interferometry utilizing phase|
|US7488930||Jun 2, 2006||Feb 10, 2009||Medeikon Corporation||Multi-channel low coherence interferometer|
|US7777940||Feb 8, 2008||Aug 17, 2010||University Of Central Florida Research Foundation, Inc.||Extreme chirped pulse amplification and phase control|
|US7876446 *||Feb 3, 2006||Jan 25, 2011||Universitat Stuttgart||Method and assembly for confocal, chromatic, interferometric and spectroscopic scanning of optical, multi-layer data memories|
|US7917039||Feb 6, 2008||Mar 29, 2011||University Of Central Florida Research Foundation, Inc.||Signal processing using spectrally phase-encoded optical frequency combs|
|US7995207||Oct 14, 2004||Aug 9, 2011||University Of Kent||Spectral interferometry method and apparatus|
|US8472027||Jul 8, 2011||Jun 25, 2013||University Of Kent||Spectral interferometry method and apparatus|
|US8655431||May 31, 2011||Feb 18, 2014||Vanderbilt University||Apparatus and method for real-time imaging and monitoring of an electrosurgical procedure|
|US9014788||Feb 18, 2014||Apr 21, 2015||Vanderbilt University||Apparatus and method for real-time imaging and monitoring of an electrosurgical procedure|
|US9129612 *||Jul 22, 2014||Sep 8, 2015||Shangqing Liu||Six-dimensional optical multilayer storage using two-photon absorption writing, erasing and optical coherence tomography reading|
|US20030045798 *||Sep 4, 2001||Mar 6, 2003||Richard Hular||Multisensor probe for tissue identification|
|US20040160611 *||Feb 14, 2003||Aug 19, 2004||Li Chian Chiu||Interferometric optical imaging and storage devices|
|US20040161165 *||Feb 20, 2004||Aug 19, 2004||Amnis Corporation||Method and apparatus for correcting crosstalk and spatial resolution for multichannel imaging|
|US20050249107 *||Jul 24, 2005||Nov 10, 2005||Chian Chiu Li||Multi-layer Optical Disc And System|
|US20050254059 *||May 14, 2004||Nov 17, 2005||Alphonse Gerard A||Low coherence interferometric system for optical metrology|
|US20050254060 *||Jan 21, 2005||Nov 17, 2005||Alphonse Gerard A||Low coherence interferometry for detecting and characterizing plaques|
|US20050254061 *||Jan 21, 2005||Nov 17, 2005||Alphonse Gerard A||Low coherence interferometry for detecting and characterizing plaques|
|US20050261568 *||May 26, 2005||Nov 24, 2005||Bioluminate, Inc.||Multisensor probe for tissue identification|
|US20070055117 *||Oct 25, 2006||Mar 8, 2007||Alphonse Gerard A||Low coherence interferometry utilizing phase|
|US20070165234 *||Oct 14, 2004||Jul 19, 2007||University Of Kent||Spectral interferometry method and apparatus|
|US20070231779 *||Feb 14, 2007||Oct 4, 2007||University Of Central Florida Research Foundation, Inc.||Systems and Methods for Simulation of Organ Dynamics|
|US20070239031 *||Apr 14, 2006||Oct 11, 2007||Kye-Sung Lee||Systems and methods for performing simultaneous tomography and spectroscopy|
|US20070278389 *||Jun 2, 2006||Dec 6, 2007||Mahesh Ajgaonkar||Multi-channel low coherence interferometer|
|US20080089641 *||Oct 3, 2007||Apr 17, 2008||Feldchtein Felix I||Optoelectronic lateral scanner and optical probe with distal rotating deflector|
|US20080151253 *||Feb 3, 2006||Jun 26, 2008||Universitat Stuttgart||Method and Assembly for Confocal, Chromatic, Interferometric and Spectroscopic Scanning of Optical, Multi-Layer Data Memories|
|US20080193904 *||May 4, 2007||Aug 14, 2008||University Of Central Florida Research Foundation||Systems and Methods for Simulation of Organ Dynamics|
|US20110092823 *||Jul 19, 2010||Apr 21, 2011||The General Hospital Corporation||System and Method for Identifying Tissue Using Low-Coherence Interferometry|
|US20150063089 *||Jul 22, 2014||Mar 5, 2015||Shangqing Liu||Six-dimensional Optical Multilayer Storage Using Two-photon Absorption Writing, Erasing and Optical Coherence Tomography Reading|
|EP1624450A1 *||Aug 6, 2004||Feb 8, 2006||CSEM Centre Suisse d'Electronique et de Microtechnique SA||Parallel OCT readout schemes for optical data-storage applications|
|WO2002086416A2 *||Apr 24, 2002||Oct 31, 2002||Amnis Corporation||Method and apparatus for correcting crosstalk and spatial resolution for multichannel imaging|
|WO2002086416A3 *||Apr 24, 2002||Feb 20, 2003||Amnis Corp||Method and apparatus for correcting crosstalk and spatial resolution for multichannel imaging|
|WO2006012760A1 *||Jul 15, 2005||Feb 9, 2006||Csem Centre Suisse D'electronique Et De Microtechnique Sa||Parallel oct readout schemes for optical data-storage applications|
|U.S. Classification||369/128, 369/94, 369/102, 369/106|
|International Classification||A61B5/00, G01B9/02, G01N21/47|
|Cooperative Classification||G01B9/02004, G01B9/02091, G01B2290/45, G01B9/0205, G01B9/02044, Y10S977/951, A61B5/0066, A61B5/6852, G01N21/4795|
|European Classification||A61B5/00P1C, A61B5/68D1H, G01B9/02, G01N21/47S|
|Jan 16, 2004||SULP||Surcharge for late payment|
|Jan 16, 2004||FPAY||Fee payment|
Year of fee payment: 4
|Jun 7, 2005||AS||Assignment|
Owner name: RESEARCH FOUNDATION OF THE UNIVERSITY OF CENTRAL F
Free format text: ASSIGNMENT;ASSIGNOR:UNIVERSITY OF CENTRAL FLORIDA;REEL/FRAME:016097/0534
Effective date: 20050606
|Nov 30, 2007||FPAY||Fee payment|
Year of fee payment: 8
|Nov 22, 2011||FPAY||Fee payment|
Year of fee payment: 12